TW574561B - Bistable nematic liquid-crystal display device with improved optical mask - Google Patents
Bistable nematic liquid-crystal display device with improved optical mask Download PDFInfo
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- TW574561B TW574561B TW091119601A TW91119601A TW574561B TW 574561 B TW574561 B TW 574561B TW 091119601 A TW091119601 A TW 091119601A TW 91119601 A TW91119601 A TW 91119601A TW 574561 B TW574561 B TW 574561B
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells
- G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
- G02F1/1333—Constructional arrangements; Manufacturing methods
- G02F1/1337—Surface-induced orientation of the liquid crystal molecules, e.g. by alignment layers
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells
- G02F1/137—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells characterised by the electro-optical or magneto-optical effect, e.g. field-induced phase transition, orientation effect, guest-host interaction or dynamic scattering
- G02F1/139—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells characterised by the electro-optical or magneto-optical effect, e.g. field-induced phase transition, orientation effect, guest-host interaction or dynamic scattering based on orientation effects in which the liquid crystal remains transparent
- G02F1/1391—Bistable or multi-stable liquid crystal cells
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells
- G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
- G02F1/1333—Constructional arrangements; Manufacturing methods
- G02F1/133371—Cells with varying thickness of the liquid crystal layer
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells
- G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
- G02F1/1333—Constructional arrangements; Manufacturing methods
- G02F1/1335—Structural association of cells with optical devices, e.g. polarisers or reflectors
- G02F1/133509—Filters, e.g. light shielding masks
- G02F1/133512—Light shielding layers, e.g. black matrix
Abstract
Description
574561574561
本發明係關於液晶顯示器的領域。 更明確地說,本發明關於雙穩態固位—破 列式液晶顯 示器,兩個穩定結構其以一〗8 η ° AA L ^ 1 6U 的杻曲不同 液晶顯示器被廣泛地利用到為電腦,影投 機,手錶及許多其他用來展現資料 ^^ :機,電視 及影像。他們的表面通常被分割為構成單體=了號,文章 素),他們的狀態是獨立的。 A小元件(像 要的品質標準是光學對比,這個 或對比比例的數量來定義。一個 將放在開啟狀態的瑩幕上一區域 ’與該同樣區域在關閉狀態下所 值(是要考慮所傳遞的或所反射# 以傳遞或反射原理操作而決定)。 想情況的特徵是,傳遞或反射的 的關閉狀態則是,傳遞或反射的 比提供所顯示的訊息成影像一更 液晶顯示器一個非常重 質通常由一 晶顯示器的 所傳遞或反 遞或反射光 光是由該顯 該顯示器的 度越1¾越好 度越低越好 被稱為對比 對比是指, 射光的強度 .之強度的比 不1§設計是 開啟狀態理 ,然而理想 。一個高對 的了閱f生及更好的比質。例如,小於1 〇的對比比例相應於 一個暗淡無光的或褪色的影像。這以一對比值20呈現的相 ,的衫像疋更梵及更明銳。假若在正常情況下觀察該顯示 态的後者尺寸,比眼睛解析度極限更小的話,該顯示器中 所考慮用來測量該對比的區域可以包含許多像素。 574561 ____索號 91119601_^-----— 五 '發明說明(2) 一個液晶顯示器通常包括,如所附的圖1到圖3中以圖示方 式所展示,兩個分別在其内表面設有電極1 〇,2 〇,而在兩 述電極之間充滿液晶物質3 0的平行的基層板1 2 ’ 2 2。該相 反電極10,20彼此交叉的區域形成該像素。所顯示的影 像是由這些被放在所要的光學狀態的大量像素所形成。每 一個像素的光學狀態,也就是說,它是否是開或關,是由 形成該像素的電極1 〇,2 0之間所施加的一適合電場及所使 用的該定址電路來決定。 大部份的液晶顯示器是單穩態的。在這些顯示器,單一結 構是在沒有電場的條件下產生。在一個電場中,這個結構 逐漸地改變’提供漸增地明亮(或漸增地關閉)狀態。 雙穩態顯示器具有至少兩種狀態,理論上在沒有外加電場 下可無限長時間下維持穩定。這兩種狀態之一是關閉狀 態,而另一個狀態是開啟狀態。這兩種狀態的穩定性基於 的事實是,這兩種結構的能量實際上是相同的,而且有一 防止一個結構自然地轉換到另一個結構的能量障礙。 相鄰的像素不是接觸的,而是被一稱為像素間區域的(參 考圖3)非可地址化的區域分隔。在圖3以圖展示具有一樣 的一像素及具標示丨的一像素間間隔。例如,當該顯示 益j個被動式距陣形式組織成時,該列電極丨〇被固貼到 一 土曰板12,該排電極2〇被固貼到另—基層板22,而電極The invention relates to the field of liquid crystal displays. More specifically, the present invention relates to a bi-stable retention-broken liquid crystal display. The two stable structures are widely used as computers with a curvature of 8 η ° AA L ^ 1 6U. Film speculation, watches and many other materials used to display information ^^: machine, television and video. Their surface is usually divided into constituent monomers (numbers, texts, primes), and their states are independent. A small component (like the quality standard to be optical contrast, this or the number of contrast ratios is defined. An area that will be placed on the screen in the open state 'and the value of the same area in the closed state (is to be considered Transmitted or reflected # is determined by the operation of the principle of transmission or reflection). The characteristic of the situation is that the closed state of transmission or reflection is that the transmission or reflection is more than providing a displayed message into an image-a liquid crystal display is a very The weight is usually transmitted or reversed or reflected by a crystal display. The degree of the display is as low as possible. The better the lower the better. It is called the contrast. The ratio of the intensity of the light. The design is not open, but it is ideal. A high quality and better quality. For example, a contrast ratio of less than 10 corresponds to a dull or faded image. With a contrast value of 20, the shirt looks more brave and sharper. If the latter size of the display state is observed under normal circumstances, the display is smaller than the eye resolution limit, the display The area under consideration for measuring this contrast may contain many pixels. 574561 ____Sorting number 91119601 _ ^ --------- Five 'description of the invention (2) A liquid crystal display usually includes, as shown in the attached Figures 1 to 3 As shown in the figure, two parallel substrates 1 2 ′ 2 2 each provided with electrodes 10, 2 0 on their inner surfaces, and filled with a liquid crystal substance 30 between the two electrodes. The opposite electrode 10 The area where 20 intersects each other forms the pixel. The displayed image is formed by a large number of pixels placed in the desired optical state. The optical state of each pixel, that is, whether it is on or off, is A suitable electric field applied between the electrodes 10 and 20 forming the pixel is determined by the addressing circuit used. Most liquid crystal displays are monostable. In these displays, a single structure is in the absence of an electric field. Generated under the conditions of an electric field. This structure gradually changes in an electric field to provide an increasingly bright (or gradually closed) state. A bi-stable display has at least two states, theoretically without an external electric field Stable for infinite time. One of these two states is off and the other is on. The stability of these two states is based on the fact that the energy of these two structures is actually the same, And there is an energy barrier that prevents one structure from naturally transitioning to another. Adjacent pixels are not in contact, but are separated by a non-addressable area called the inter-pixel area (see Figure 3). In Figure 3 The figure shows a pixel with the same interval and a pixel-to-pixel interval. For example, when the display is organized into passive matrix patterns, the columns of electrodes are fixed to a soil plate 12, which The row electrode 20 is fixed to the other base plate 22, and the electrode
第7頁 574561 案號 91119601 五、發明說明(3) 10及20以90度彼此交叉安置 該區域包圍,在此區域中該 豐’而且該像素間的這些間 之那些區域’不管這是在該 這個電極間的空間可使每_ 它不會被降低到一由構成該 的钱刻技術,及該顯示器其 下。 。在這種案例中,該像素p被 列電極1 0及排電極2 0彼此重 隙ί相應於面對一電極間空間 列基層板1 2或該排基層板2 2。 #電極與其鄰居分隔開,而且 1:極材料本質及厚度及所採用 他特性所決定的一關鍵值以 在沒有一阻礙層存在時, 的,而且由這些區域所傳3素間間隔的光學狀態是不好 對比性質大大地降低。例如或反射的光可能使一顯示器的 0.23龍邊長的正方形像夸如/—個以具有螺距及 為〇.〇2 像素間間隔象的顯示器,將有一個寬度 作區域1 5%的一個完全不朴子應於大約等於該瑩幕全部工 呈開啟的不利情況下,兮作驻用區域。在一個像素間隙永遠 中所測量到之對比可处Ϊ顯示器在一包圍幾個像素的區域 該像素中所測得的要低的一數值,即使在 做小對比是很高的。 使用一個負對比顯示模 關閉狀態的一種楔式,、f(也就是,當電場是零時,具有 式),可使限制相較於—列如在平行極性元件中的以模 能。但是,這個解決方正曰對比顯示器的對比損失成為可 、万木是不能應用到高解析度顯示器,Page 7 574561 Case No. 91119601 V. Description of the invention (3) 10 and 20 cross each other at 90 degrees to surround the area, in which the area is' rich 'and the areas between the pixels are' regardless of whether it is in the area The space between this electrode can make it not lowered to a composing technology and the display underneath. . In this case, the pixel p is spaced from each other by the column electrode 10 and the row electrode 20 corresponding to the space between the electrodes, such as the column base plate 12 or the row base plate 22. #Electrode is separated from its neighbors, and 1: the key material determined by the nature and thickness of the polar material and the other characteristics used in order to prevent the presence of an obstacle layer The state is bad and the nature of the contrast is greatly reduced. For example, or the reflected light may make a 0.23 long square image of a display exaggerate / a display with a pitch and a pitch interval of 0.02 pixels, which will have a width of 15% of a complete area. Bu Puzi should be used as a resident area under unfavorable conditions that are approximately equal to the opening of all the curtains. The contrast measured in a pixel gap is always good. The display is in an area surrounding several pixels. The measured value in this pixel is a low value, even when the small contrast is high. Using a negative contrast to display a mode of wedge, f (that is, when the electric field is zero, has a formula), can make the limit compared to the column mode in parallel polar elements. However, this solution found that the contrast loss of the contrast display becomes acceptable, and Wanmu cannot be applied to high-resolution displays.
574561 修正 7 又 W - Ξ Ξ 2、ϊ在該像素定址時所產生的橫向電場將使鄰近電 s 、乂晶結構扭曲,並且將其轉成光學上開啟狀態 負對比也許同樣需要使用—個不利的^ 壯離I兰”有負對比TN的關閉狀態比具正對比”的關閉 示ί的對比因為它的色收差(Chr_tiSffl),因此限制了顯 ,他所有為了緩和因瑩幕的該不作用部份所 辦法,皆在像素之間或在該電 止光傳遞或反射之不透明層為基礎。 i ΐ 出使用铭或絡層當光罩。使用金屬當光罩 路的二二過程及防止在像素之間出現短 可降層同樣有一大約在h5到3%的不 降低的反光度,藉此而限制反射時的對比。 m〕曰提出λ用二吸收(彩色的或黑色的)高分子充當 一疋°玄%色尚分子的低光學密度使他們的使用厚 對的厚(>0.5 "m),為了要獲得一足夠二 钟1%)。將這些層面蝕刻因此會在顯示器内產&生突 如r帶的非均勻的電場的出現它會誘發 放大以便部份遮蓋電極^\扭^轉區域。如果將光罩 的狀態中會對光的ί 2=::些瑕疵可以減低,在開 ’、及反射造成的損害。此外,對這些574561 Correction 7 and W-Ξ Ξ 2, ϊ The lateral electric field generated when the pixel is addressed will distort the adjacent electric s and crystal structure and turn it into an optically open state. Negative contrast may also need to be used—a disadvantage ^ Zhuangli Ilan "The closed state of negative contrast TN is better than the closed state of positive contrast" because of its poor color reception (Chr_tiSffl), it limits the display. All methods used in the function are based on the opaque layer between the pixels or the electric stop light transmission or reflection. i ΐ Use the mask or envelope as a photomask. The second and second process of using a metal as a photomask and preventing shorts between pixels can also have a non-reduced reflectance of about 5 to 3%, thereby limiting the contrast during reflection. m] said that λ uses bis-absorbent (colored or black) polymers to act as a 疋 ° %% color molecule. The low optical density makes them use thick pairs (> 0.5 " m). Enough for two minutes 1%). Etching these layers will therefore produce & generation of non-uniform electric fields such as r-bands in the display. It will induce magnification to partially cover the electrode ^ \ twisting ^ area. If the state of the reticle is lightened to 2 = :: some blemishes, the damage caused by opening and reflection can be reduced. Also, for these
第9頁 ^/4561Page 9 ^ / 4561
修正 &疋很差的^這代表 維持足夠的準位。這 示器的其他的重要性 光罩 些方 質有 非常厚的聚合物層的蝕刻的 必須加寬以便在光罩及電極之 =因此維持該對比,但是對該顯 害,它就是照明狀態的亮度。, 另一個解決方案是採用一由一 抗-反光及隔離功能〔4〕的吸=遮撞層及-用來提供 的傳送及反射的光學性質最優卜合物層’如此可使光罩 度,或使用其5审〜她以又化,而沒有過度地增加其厚 當4锄冬®^複濰的,包含具有吸收性質〔5〕的非 “ ·致金屬或半導體粒子的電介^基楚的結構。 :有料$方法包括了額外的製造操作及使用了昂貴材料 I過私。坆疋因為必須將不透明的材料沈澱到電極上並將 /、由該活動的(active)區域中去除。這些操作必須精準, 因為它必須在不侵犯像素或造成非阻礙區域的條件下建立 〇·〇1或0·02 mm寬度的不透明帶。所花費的額外費用在被 動距陣顯示器的案例中特別是高的無人問津,sTN_LCD單 色顯示态可為它的參考價格,而且它的製造過程沒有使用 真空沈澱。 以雙穩態向列液晶單體的案例中,利用修改或改良該製造 操作可使本發明不使用添加物質使像素間空隙被遮蓋 (block of f)。它使用雙穩態顯示器的性質,這些性質將 簡單地回顧一下。Correction & 疋 Poor ^ This means maintaining a sufficient level. This shows the other importance of the photomask. Some of the substrates have a very thick polymer layer. The etching must be widened so that the contrast between the photomask and the electrode is maintained, but to the detriment, it is the lighting state. brightness. Another solution is to use an anti-reflective and isolating function [4], an absorption = shielding layer, and-an optimal composite layer used to provide the optical properties of transmission and reflection. , Or use its 5th trial ~ she re-evaluated without excessively increasing its thickness. 4 锄 冬 ® ^ Fu Wei's, containing a non- "metal- or semiconductor-containing dielectric group with absorption properties [5] Chu's structure: The method includes additional manufacturing operations and the use of expensive materials. It is because the opaque material must be deposited on the electrode and / or removed from the active area. These operations must be precise, as it must create opaque bands with a width of 0.001 or 0.02 mm without infringing pixels or causing unobstructed areas. The additional cost incurred is particularly so in the case of passive matrix displays. Highly unknown, the sTN_LCD monochrome display state can be its reference price, and its manufacturing process does not use vacuum precipitation. In the case of a bistable nematic liquid crystal monomer, by modifying or improving the manufacturing operation, Invention does not use substances added to make the inter-pixel gap is covered (block of f). It uses the properties of bi-stable display, these properties will be briefly review.
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修正 «^4 板上的八 1 6〕提出一雙穩態顯示器,其狀態是以基層 位)。子同&樣平的或幾乎平的位置所造成(單穩態固 呈現不二狀態在基層板的兩個表面之間以其液晶結構而 (該結播同曰。在其中之一的狀態中,該分子實際上是平行的 以半·链疋均勻的或稍微地扭曲)。在另一個狀態中,分子 原先的結圈M轉H面的’由一基層板到另一基層板(相對於 的轉換、"Η “、·Ό構以1 8 0。被扭曲)。在這兩個結構之間 至少在复疋在強烈電場中利用一流體動力效應方式破壞 一中之一表面上的該單穩態固位而獲得。 2 ί ί :巾’像素間的空間利用產生雙穩態單體而遮蓋, 用將素之間空隙令的液晶呈永遠地關閉狀態。這是利 自然扭曲條件設定成特別適合於覆蓋在像素 盥接二鬥日日層,如此在其中對提供關閉狀態結構有利, 二:二bn 狀態的結構相較,這些情況降低它 厶剞顧,、哭沾假設用來觀察在傳遞型,反射型或在-個混 二產生二二叮光極化組態最適化的目標,是朝向能在像素 應!構或該均句結構。舉例說明,在反光型態二 極化^的㈣化最好是依照本 日提出临惠關7專利中請案中所以的規定來=Modification «^ 4 on the board 8 1 6] proposed a bistable display whose status is at the grassroots level). It is caused by the & sample flat or almost flat position (the monostable state is a solid state between the two surfaces of the base plate with its liquid crystal structure (the conclusion is the same. In one of the states In this case, the molecule is actually parallel or evenly twisted with a half chain.) In another state, the molecule's original knot M to H plane is' from one base plate to another base plate (relatively The conversion of Yu, "Η" is structured with 1 8 0. Distorted). Between these two structures, at least in a strong electric field, a hydrodynamic effect is used to destroy one of the surfaces. The monostable position is obtained. 2 ί ί: The space between the pixels is covered by the production of a bistable monomer, and the liquid crystal is closed permanently by the gap between the elements. This is a natural distortion condition It is set to be particularly suitable for covering the two layers of the pixel toilet, so it is beneficial to provide a closed state structure in it. Second: Compared with the structure of the two bn states, these conditions reduce it to ignore, and cry Observe in transitive, reflective or mixed The goal of optimizing the optical polarization configuration of the two-two-biter is to aim at the pixel structure or the uniform structure. For example, it is best to propose Linhui according to today's proposal based on the reflection of the two-polarization in the reflective form. All the requirements in the 7 patents are filed =
第11頁 574561Page 11 574561
曰 修正Correction
依據本發明’該雙穩態向列液晶顯示器包括用來 素間光罩: /成~像 a) —限制在兩平行基層板之間的向列液晶物質, 在該基層板相對的内表面上設置有電極,用以施加一電p 到該液晶上’至少該前基層板及該前電極是光學透明^野 b )準位層或用以將液晶導向定位,以及至少’ 個穩定的或在沒有電場下,呈亞穩的明顯結構之間產=, 迭的電極上所做的處理,其中該結構之一是不被扭曲 或通過在一 90。及+90。之間的一角度呈被扭曲的卜, 況,而另一,結構具有一大約18〇。角的額外的扭曲^ c)覆盍該電極液晶層的厚度4選擇的方式是要 Δη的乘積接近;或,接近整數乘以波長戈^ 二於ί ΐ個數值之間(要看該顯示器的操作模式是反射/、 遞型的或傳遞反射型的),又。是該顯示器有用 碏页中間波長,而Δη &對此波長的液晶的雙折射率的先 二:計用來對覆蓋該電極的液晶施加電力訊號 ί號可使液晶在該明顯的結構之間轉換,ili ;;二去⑨之後使其仍維持在其中之-的結構,這是利; 破壞在至少該兩個基層板之一上的固位而達成; e)設計用來增進覆蓋該電極間空間的液晶中產生# 關閉狀態結構之一的建立。 丫座生。兹 1與Γ須了解極化件的數量及排列的最佳化是依照顯示 益光子細作模式(傳送式的’反射式的或傳遞反射型的)。According to the invention, 'the bi-stable nematic liquid crystal display includes a photomask for prime elements: / formation ~ image a)-a nematic liquid crystal substance confined between two parallel base plates on the opposite inner surface of the base plate An electrode is provided to apply an electric p to the liquid crystal 'at least the front base plate and the front electrode are optically transparent b) a leveling layer or used to orient the liquid crystal, and at least' stable or In the absence of an electric field, a metastable apparent structure is produced between the electrodes. One of the structures is not distorted or passed through a 90 °. And +90. One angle between them is distorted, while the other has a structure of about 180 °. Additional distortion of the angle ^ c) the thickness of the electrode liquid crystal layer 4 is chosen to be close to the product of Δη; or, close to the integer multiplied by the wavelength, ^ 2 to 数值 a number (depending on the display's The operation mode is reflective / transmissive or transflective), again. It is the middle wavelength of the useful page of the display, and Δη & the first two of the birefringence of liquid crystals at this wavelength: the meter is used to apply a power signal to the liquid crystal covering the electrode. The liquid crystal can be placed between the obvious structures. Conversion, ili ;; the structure of which is still maintained in it after the two are removed; this is beneficial; it is achieved by destroying the retention on at least one of the two base plates; e) designed to improve the coverage of the electrode The creation of one of the # off-state structures in the interstitial liquid crystal. The girl is born. Hereby, 1 and Γ must understand that the number and arrangement of polarizers are optimized in accordance with the display photon fine-grained mode (transmissive 'or reflective type).
574561574561
依本發明的其他的優勢特點: 使在相同in 2中之一包含有幾個不同的部份,為了 素(像素)成^可能;,相層板上產生幾個獨立的圖像元 式距陣; 式距陣; 該電場;該獨立的圖像元素(像素)設有獨立的裝置可施加 I該獨立的圖像元素(像素)可被組織成多種的被動 ;該獨立的圖像元素(像素)可被組織成多種的主 多的特點’目的及優點,在閱讀結合所附帶用來 楗仏非限制性例子的圖示的該詳細描述後會變得更明確, 其中; 構成本發明主題的顯示器可以在覆蓋他們像素的液晶居^ 址兩個穩疋的結構。在該液晶中加入一種可產生螺旋線 濃液(chiral dopant)就可獲得雙穩態性質。 。、,、、> 之 沒有一可產生螺旋線濃液時,一液晶在沒有扭力之情況 具有一均勻的方位定向。它的自由螺距是無限的。=二了 產生螺旋線濃液存在時,當液晶沿著它的軸向通過時,: 液晶的方位沿著它的螺旋線轉動。這樣的話該液曰°目 χ α曰曰具一有 限的自由螺距(在沿著它的軸位移與該螺距相笨 〒距離According to the other advantages of the present invention: one of the same in 2 contains several different parts, in order to make it possible for the pixel (pixel); several independent image element distances are generated on the phase plate The array; the distance array; the electric field; the independent picture element (pixel) is provided with an independent device that can be applied; the independent picture element (pixel) can be organized into a variety of passive; the independent picture element ( (Pixels) can be organized into a variety of features. The purpose and advantages will become clearer after reading this detailed description in conjunction with the accompanying illustrations for non-limiting examples, where: The display can have two stable structures in the LCD covering their pixels. Adding a chiral dopant to the liquid crystal can obtain bistable properties. . When there is no one that can produce spiral dope, a liquid crystal has a uniform azimuth orientation without torque. Its free pitch is infinite. = Two. When the concentrated liquid with the spiral line exists, when the liquid crystal passes along its axis, the orientation of the liquid crystal rotates along its spiral line. In this case, the liquid is °°, χ α, and has a limited free pitch (the distance along the axis is staggered with the pitch).
第13頁Page 13
574561 ---- 案號 9H19601_主一^修正 五、發明說明(9) 後,該方位方向轉動360。)。當濃液濃度增加時,該自由 螺距減低。液晶的自由扭曲qG是以2 7Γ /Pq的表述來定 義’其中PQ是液晶的自由嫘距’對具有厚度d的該液晶的 一樣品檢驗之後得知,該自然扭曲是由d · 定義的。在 沒有任何力矩的情況下,對該液晶層做檢驗之後得知,該 自然的扭曲因此是該方向件已經轉動的角度。 雙穩態性質是利用調整覆蓋在該像素上該液晶厚度中自然 扭曲到一 9 0 °數值而獲得。在表面上固位的條件,在兩個 可能-扭曲的及均勻的—結構指示該液晶以相對於它的平衡 狀態大約90。扭曲變形。那麼這兩個狀態是相等的及這兩 個〜構i成雙穩態。這兩種狀態的能量因此相同而這兩種 結構變成雙穩態。一小於9〇。的自然扭曲有利於該均勻結 構,而^ 一方面一大於9〇。的自然扭曲有利於該扭曲結 構在這個1¾段我們應注意在該表面上固位的良好特質同 樣也對該結構的能量。例如對在該單體厚度中的液晶的9〇 的自然扭曲,一具有足夠高的平行預傾角的固位組態將 有利於該扭曲結構’然而有相同的但非平行預傾角的組態 :ΐ ί均勻結構。在實際情形下,為了保證雙穩態, 衡不是絕對必要的,因為存在-可防止由- 、,,口構,移轉到另一結構的位能阻礙。例如,該自然扭曲 $中心的一某一範圍中做調整而不會喪失雙 ^ 曲的及均勻結構兩者皆為穩定的)。但是,在 此範圍之外,該最低能量的結構是唯一穩定的(參考圖574561 ---- Case No. 9H19601_Main ^ Amendment 5. After the description of the invention (9), the azimuth direction rotates 360. ). As the dope concentration increases, the free pitch decreases. The free distortion qG of a liquid crystal is defined by the expression of 2 7Γ / Pq, where PQ is the free pitch of the liquid crystal. After examining a sample of the liquid crystal having a thickness d, it is known that the natural distortion is defined by d ·. In the absence of any moment, after examining the liquid crystal layer, it is learned that the natural distortion is therefore the angle at which the directional member has been rotated. The bistable nature is obtained by adjusting the natural distortion of the liquid crystal thickness over the pixel to a value of 90 °. The conditions for retention on the surface, in two possible-distorted and uniform-structures, indicate that the liquid crystal is about 90 in equilibrium with respect to it. Distortion. Then these two states are equal and the two ~ are constructed into a bi-stable state. The energy of these two states is therefore the same and the two structures become bistable. One is less than 90. The natural distortion of is beneficial to the uniform structure, while ^ is greater than 90 on the one hand. The natural distortion of B is beneficial to the twisted structure. In this section, we should pay attention to the good characteristics of retention on the surface as well as the energy of the structure. For example, for the natural distortion of 90 ° of the liquid crystal in the thickness of the monomer, a retention configuration with a parallel pretilt angle that is sufficiently high will be beneficial to the twisted structure ', however, the configuration with the same but non-parallel pretilt angle: ΐ ί uniform structure. In actual situations, in order to ensure the bi-stable state, the balance is not absolutely necessary, because the existence-can prevent the transfer of the structure from the-to the structure of the energy barrier. For example, the natural distortion $ is adjusted in a certain range of the center without losing both the hyperbolic and uniform structure). However, outside this range, the lowest energy structure is the only stable (refer to the figure
第14頁 574561 修正 案號 91119601 _ ^ 日 五、發明說明(1〇) 4) ° 由本發明所發展出的裝詈,闲α A ,步„ 衣直用以在覆盍像素間隙之液晶建 立產生關閉狀態的結構現在將提出。 第一種裝置 不同的液晶 加物質來調 為了是要使 層板的電極 液晶厚度令 覆蓋在像素 地方的扭曲 性將喪失而 個差異足夠 所有需要的 該產生開啟 均勻結構或 假若它是產 電極間空間 立它,因此 厚度, 整。因 其中的 之間空 在該像 及該像 與90 ° 兩個結 造成對 是在製 狀態的 扭曲% 這個厚 為在像 該扭曲 間的局 素間隙 素之間 理想平 構之一 一結構 造時設 結構不 結構’ 非活動區(像素間之間隙)中產生 度差異是利用選擇性的去除或增 素的自然扭曲必須接近到9 0。, 及均勻結構能量相等,在每一基 部增加或去除物質減少或增加在 中的該自然扭曲。扭曲的差異與 間隙中液日日厚度成正比。當一個 衡扭曲呈顯著的差異時,雙穩定 呈優勢(例如大約5。到1 〇。的一 有利)。依照此第一裝置,因此 定該所說的厚度差異為一足夠使 穩定的數值(這個結構有可能是 視所採用的偏光模組態而定)。 的::狀態的扭曲結構,在至少-個基層板上 开=。凹隙有利於它並且可在像素間隙之間建 化成—液晶光罩(參閱圖5)。 右匕疋產生關閉狀態的均勻結構 在電極間的局部材料Page 14 574561 Amendment No. 91119601 _ ^ 5th, description of the invention (1〇) 4) ° The device developed by the present invention, leisure α A, is used to create and generate liquid crystals covering the pixel gap. The structure of the closed state will now be proposed. The first device uses different liquid crystals to add materials to adjust the thickness of the electrode liquid crystals of the laminate so that the distortion of the pixel area will be lost, and the difference is sufficient for all the required to generate the uniform opening. The structure or if it is a space between the electrodes, it is thick and uniform. The space between the image and the image and the 90 ° two junctions cause the distortion in the control state. The thickness is in the image. Local gaps between twists One of the ideal flat structures between primes-structure and time, structure is not structured 'The difference in degree of generation in the inactive area (gap between pixels) is that the natural distortion using selective removal or enrichment must be close To 9 0., and the uniform structural energy is equal, adding or removing matter at each base reduces or increases the natural distortion in the. The difference between the distortion and the liquid day in the gap The thickness is directly proportional. When a balance distortion has a significant difference, the bi-stable is advantageous (for example, an advantage of about 5. to 10). According to this first device, the thickness difference is determined to be a sufficient Stable value (this structure may depend on the configuration of the polarizing mode used). :: The twisted structure of the state, opened on at least one base plate =. The recess is favorable for it and can be in the pixel gap. Indirect formation—a liquid crystal reticle (see Figure 5). The right dagger produces a closed structure of the uniform material between the electrodes.
574561 θ —案競911〗恥ηι 五、發明說明(11) 沈澱,至少在一基層板上 6) 〇 修正 可達到相同的結果(參閱圖 例如,讓我們以反光型顯示器為 在後面設有-反射器,該顯;器:充滿了具有 又/ Ω 0· 13。覆蓋該像素的液晶厚度d被選為1. 1 Γ:兮、U型最大厚度相等,其公式為d ·一一又-其中 一.11曰呆作區域的中間波長。該扭曲結構因此產生關 :":。。對該像素產生雙穩態的自然平衡扭曲在製造時調 -到90 。利用在每一基層板上的電極間空間設一 〇1 1 ^ 在覆盍在像素間間陷的液晶厚度中該自然扭 曲變成大約9 8。(相辇於】9 ,, 丄 ^ ^ - ΛΛ ^ ,相4於1 · 2 // m -在此我們忽略了兩個基 父的電極間空間的小區域的例子)。這個扭曲足夠 反射度的關閉狀;:光以個環繞該像素而具有低 像责中、:B ί Ϊ間之間隙中液晶厚度必須維持足夠接近 該‘閉2 Si : I ί二如此該像素間隙中的光學狀態將維持 的厚产的:昱.I Ϊ盍該像素的液晶厚度與該像素間之間隙 i 乂又、又有超過覆蓋該像素液晶厚度的大約1 5 % , 被滿足。這個條件確定了顯==隙 間準位表面的振在該電極上或電極間空 在電極間工間廷擇凹陷或添加物質,而且蝕刻或沈澱方法 第16頁 574561 月 曰 修正 茶號 91119601 五、發明說明(12) 的選擇要考慮是否與慣用生產顯示器的 如,假若使用一電漿蝕刻裝置來生產電’,泰配。例 輕微凹陷既不需要一額外的光罩也不需要一::::間的 (但是,有可能需要修改蝕刻係數)。 ,的知作過程 由本發明所發展出用以形成液晶光罩的另一 到本案例’其中該關閉狀態是該扭曲結構所產二置被應用 置包括製造具有可建立隙槽厚度的電極,允 =個裝 在該像素間間隙中被建立起來。作是 :二曲結構 i日蚪/1 ΛΑ + k ,丨 疋 义個方法需要fi、生 相對;的電極(例如厚度大約在4〇⑽ I k 個無法與該顯示器的光學 < 電學上夕)有時候這 限制相匹配。…成…的規格或與-些製造上 另外一個用以誘 螺旋線濃液的成 結構為止,該顯 的液晶厚度稍微 能障礙事實上對 提供了某一限制 增加到一接近在 點。任何凹陷的 使是很不顯著, 夠可選擇性地在 螺旋線濃液成份 么忒液晶光罩的方法是調整該液晶可產生 份1一直到在像素間之間隙中出現所要的 不器被設計要使覆蓋該像素及像素間間隙 不同。存在於該扭曲及均勻結構之間的位 像素中的雙穩定性匹配的自然扭曲的範圍 _。例如,該可產生螺旋線濃液的成份可以 該像素中雙穩態的極限而沒有超越它的一 隙槽’在像素間間隙中與該像素相較,即 也可使該自然扭曲超越此限制,因此它足 其中建立該扭曲結構。利用降低該可產生 到該限制值,可將相同的方法應用到在具574561 θ — case bid 911 〖5. 5. Description of the invention (11) precipitation, at least on a base board 6) 〇 Correction can achieve the same result (see the figure for example, let's take a reflective display as the back- Reflector, the display; full: with / Ω 0 · 13. The thickness d of the liquid crystal covering the pixel is chosen to be 1. 1 Γ: Xi, U-shaped maximum thickness is equal, the formula is d · one by one- One of them is the mid-wavelength of the dull region. This distortion structure is therefore related to: ": The natural balance distortion that produces the bi-stable state of the pixel is adjusted at the time of manufacture-to 90. It is used on each substrate. The space between the electrodes is set to 10 1 ^ in the thickness of the liquid crystal covering the interstitial space between the pixels. This natural distortion becomes about 9 8. (compared to) 9,, 丄 ^ ^-ΛΛ ^, and phase 4 to 1 · 2 // m-Here we ignore the example of a small area in the space between the electrodes of the two base fathers.) This distortion is a closed form with sufficient reflectivity;: light surrounds the pixel with a low image duty,: B ί The thickness of the liquid crystal in the gap between the two must be kept close enough to the 'close 2 Si: I The optical state in the gap will be maintained in high yield: Yu.I Ϊ 盍 the thickness of the liquid crystal of the pixel and the gap i between the pixel and the thickness of the liquid crystal which covers the pixel are about 15%, which is satisfied. This The conditions determine that the apparent surface level of the gap is on the electrode or the space between the electrodes is used to pit or add materials, and the method of etching or precipitation is on page 16574561. Modified tea number 91119601. V. Invention The choice of note (12) should consider whether it is the same as the conventional production of display. For example, if a plasma etching device is used to produce electricity, Taiping. For example, a slight depression requires neither an additional photomask nor a :::: (However, it may be necessary to modify the etching coefficient.) The known process developed by the present invention to form a liquid crystal photomask to this case 'where the closed state is produced by the twisted structure is applied The setup includes manufacturing an electrode with a buildable gap thickness, allowing = one to be installed in the gap between the pixels. The operation is: the two-curved structure i 日 蚪 / 1 ΛΑ + k, which requires fi Electrodes (such as the thickness of about 40 ⑽ I k can not match the optical < electrical aspect of the display) sometimes this limit is matched to the specifications of ... or to some other manufacturing Until the formation of the helix-concentrated dope, the thickness of the displayed liquid crystal can slightly hinder the fact that it provides a certain limit to increase to a point near the point. Any depressions are very insignificant and can be selectively in the helix. The method of the thick liquid component and the liquid crystal mask is to adjust the liquid crystal to produce a portion 1 until the desired device appears in the gap between the pixels. It is designed to make the pixel and the gap between the pixels different. The range of natural distortion of the bistable match in the bit pixel that exists between this distortion and the uniform structure. For example, the composition that can generate the helix thick liquid can be the limit of the bistable state in the pixel without exceeding its gap. 'Compared with the pixel in the gap between pixels, that is, the natural distortion can also exceed this limit. , So it is enough to build the twisted structure. By reducing this to the limit, the same method can be applied to
IH 第17頁 574561 五、發明說明(13) """""""" ' ^^^9_修正 有-突出隙槽的像素間間隙— W建立該均勻結構 另外一個方法,特别是 μ 態結構的空間上的液晶層形間,利於提供關㈣ 以一種方式沈澱在該液相中成如t條件。例如,準位層可 相較,在凹陷的電極間空間内^在電極表面上其厚度 減低其方位角之固位能量。=有一額外的厚度,因而 的表面上到刷力量的局部降,與施加在這些四陷 位方向受由液晶層施加的位::結合’有利於利用方 曲結構。矛!用對該顯*器的_ 的影響滑動而建立扭 加強。也可能利用在兩個狀離中^ = f,逆個結果可以被 於在該電極間空間的方位方向的選的處理,以對 勻的結構。以同樣的方式利於其中杻曲的或均 獲取相同的結果。 ' 的選擇性的修正可以 表後’使用暫時的處理可分耸与p =間用 “I;二!於:Γ的' 充滿比夜:]如=顯示器被 :時有利於被建立在該像素中 的間隙中的該凹隙足夠大,已經觀察到的是;;:::: 第18頁 麵 574561 ----MM 五、發明說明(14)IH P.17 574561 V. Description of the invention (13) " " " " " " " " '^^^ 9_Fix the gap between pixels with -protruding gaps — W to build the uniform structure Another method, especially the interlayers of liquid crystals in the space of the μ-state structure, is conducive to providing the key to precipitate in this liquid phase in a manner such as t conditions. For example, the leveling layer may have a reduced thickness on the surface of the electrode in the recessed inter-electrode space, which reduces the retention energy of its azimuth. = There is an extra thickness, and therefore the local drop in brush force on the surface, and the bit applied by the liquid crystal layer in the direction of these four trapped positions :: combination 'is conducive to the use of a curved structure. spear! Swipe with the effect of _ on the display to establish torsional reinforcement. It is also possible to use ^ = f in the two states. The inverse result can be used to select the azimuth direction of the space between the electrodes to align the structure. In the same way it is beneficial for those that are warped or both to get the same result. The selective correction of 'can be used after the table' to use a temporary process that can be distinguished from p = "I; II! Yu: Γ's full night:] such as = display is: when it is beneficial to be built on this pixel The recess in the gap in is sufficiently large, what has been observed is;; ::: Page 18 574561 ---- MM V. Description of the invention (14)
疋不穩定的,而該扭曲的結構e古彳 “列如當它是由厚的電極银二疋迭有::的丨。假如凹陷續 ^ ^ ^ s „, /Λ40 nm) 5 ^# 所建立的扭曲狀態。這個狀態不 :=由臨時處理 影響,而就可獲得-個明確的::被接下去的顯示程序所 顯示器進行一熱處理,時 另外一個裝置是在填充之後對該 常可獲取相同的結果。 當以上所說明之一的方法被使用,杰曰 , ^ , 皮使用液晶本身將該顯示器非 -可地址化的區域阻隔並且形成一、游S伞罢土 〜风 液日日先罩,輕易獲得一 大於幾十的對比值。 無論該操作是傳遞型,反射型或傳遞反射型可獲得這個自 我-準位的液晶光罩的有利性質,而且他們與其他已經討 論過的遮蓋技術相較具有許多的優點,其中不透光層被沈 殿及餘刻: -該液晶光罩的低本質的傳遞及反射度,這些適 用來生產高對比的傳遞的,反射的或傳遞反射的顯示器; -利用一個增加的光罩來部份遮阻該像素而使關 閉狀態中沒有降格發生; 9p -在該顯示器中電場的同性沒有降格發生; -在該影像更新週期之外沒有液晶準位的干擾, 因此當此儲存的影像被觀察時對比沒有降格情況發生,·疋 is unstable, and the twisted structure e 彳 "when it is composed of a thick electrode of silver and 有: 丨. If the depression continues ^ ^ ^ s„, / Λ40 nm) 5 ^ # Twisted state established. This state is not affected by the temporary processing, but a clear one can be obtained: the display is subjected to a heat treatment by the next display program, and another device can often obtain the same result after filling. When one of the methods described above is used, Jie said, ^, the LCD uses the liquid crystal itself to block the non-addressable area of the display and form a U-shaped umbrella to cover the wind and liquid. A contrast value greater than a few tens. Whether the operation is transmissive, reflective or transflective, the self-level liquid crystal reticle has the advantageous properties, and they have many advantages over other masking technologies that have been discussed, including the opaque layer Shen Dian and the rest of the time:-The low transmission and reflectivity of the LCD mask, these are suitable for producing high contrast, transmissive, reflective or transflective displays;-using an additional mask to partially block This pixel causes no degradation to occur in the off state; 9p-no homogeneity of the electric field occurs in the display;-there is no interference from the liquid crystal level outside the image update period, so there is no contrast when this stored image is observed Degradation occurs,
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-液晶光罩沒有沈澱或準位的操作。 雖然以上的方法是以被動矩 們可以被應用到該兩基層板 中’其結果是形成可地址化 域(像素間間隙)。 陣形式的顯示器為例提出,他 的任何特別排列的電極案例 區域(像素)或非-可地址化區-No precipitating or leveling operation of the LCD mask. Although the above method is based on passive moments, they can be applied to the two base-boards. As a result, an addressable domain (inter-pixel gap) is formed. Array display as an example, any particular arrangement of his electrode area (pixels) or non-addressable area
〔1〕 A· Lien,” 一 90度TN-LCD單體的二維橫向場效的模 擬’’ ’It)RC Eurodisplay ’90 Digestif〕 歐洲專利EP 0532 311(Scheffer) 17/03/1993 年出 刊· 〔3〕美國專利 US 5 307 1 89 (Nishiki) 26/04/ 1 994 年出 刊· 〔4〕美國專利US 5 666 177(Hsieh Ting-Chang) 09/09/ 1 997 年出刊. 〔5〕美國專利 US 5 686 980 (Kobayashi) 1 1 / 1 1 / 1 997 年 出刊. 〔6〕法國專利號碼 2 740 894 (Durand).[1] A. Lien, "Simulation of two-dimensional lateral field effect of a 90-degree TN-LCD unit" 'It) RC Eurodisplay '90 Digestif] European Patent EP 0532 311 (Scheffer) 17/03/1993 Publications: [3] U.S. Patent No. 5 307 1 89 (Nishiki) published on 26/04/1. [5] US patent US 5 686 980 (Kobayashi) published 1 1/1 1/1 997. [6] French patent number 2 740 894 (Durand).
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.^ 圖1如以上所描述,以圖像展示在兩個相互垂 直的電極交叉點所獲得的一個傳統像素; 圖式簡單說明 ^ 圖2如以上所描述,以圖像展示一由雨棑交叉 :5 ί 口所構成的多種的距陣,該電極被安放在-液晶物 質的母一邊,形成像素及電極間的空間; •圖3,同樣如以上所描述,以圖像展示一這樣的 多種的距陣的剖面圖; 圖4以圖像展示該結構的穩定性以液晶厚度中 自然扭曲為相應的一函數; •圖5 ’以圖像展示在一像素間間隙中依照本發明 巧一扭曲結構,利用將物質去除,導致在該像素中 ^疋的平行(Ρ〇或扭曲的(Tw)結構(因此導致一不釋定 性)及在該像素間間隙中產生-特優的杻曲結構;且 β π 圖6以圖像展不依照本發明在一像素間隔間空間 =-平行的結構,利料加物質,導致在 = $穩疋的平行(Ρα)或扭曲的⑺)结構⑼ 。產 性)及在該像素間間隙中產生一特優的平行結構。^ 圖號說明: 4 # f ...... . 10’ 20 液晶物質.....30 基層板......12, 22 像素....4〇. ^ Figure 1 As described above, a traditional pixel obtained at the intersection of two mutually perpendicular electrodes is displayed as an image; the diagram is briefly explained ^ Figure 2 is described above as an image showing a cross by rain : 5 various arrays formed by the mouth, the electrode is placed on the mother side of the liquid crystal substance to form a space between the pixel and the electrode; Figure 3, also as described above, shows such a variety of images A cross-sectional view of the matrix; Figure 4 shows the stability of the structure in an image, with natural distortion in the thickness of the liquid crystal as a function of the corresponding function; Figure 5 'shows an image in a gap between pixels in accordance with the present invention. Structure, using the removal of matter, leading to a parallel (PO or twisted (Tw) structure in the pixel (hence leading to an indeterminacy) and a highly optimized curvature structure in the gap between the pixels; And β π FIG. 6 shows an image in accordance with the present invention. The structure of a one-pixel space = -parallel structure, adding material to the material, results in a stable (parallel (Pα) or twisted ⑺) structure =. Productivity) and produce a superb parallel structure in the inter-pixel gap. ^ Explanation of drawing number: 4 # f ....... 10 ’20 liquid crystal material ..... 30 base board ... 12, 22 pixels .... 4〇
間隙」 像素..···;;;;P"Gap" pixels ..... ;;; P
LCD分子呈平杆姓接 D 仃、、·。構· · · Pa LCD分子呈扭曲結構··The LCD molecules have a flat-bar surname followed by D 仃 ,, ·. The structure of Pa LCD molecules is distorted ...
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FR0111227A FR2829244B1 (en) | 2001-08-29 | 2001-08-29 | NEMATIC LIQUID CRYSTAL BISTABLE DISPLAY DEVICE WITH IMPROVED OPTICAL MASK |
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TW574561B true TW574561B (en) | 2004-02-01 |
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TW091119601A TW574561B (en) | 2001-08-29 | 2002-08-28 | Bistable nematic liquid-crystal display device with improved optical mask |
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US (1) | US7088413B2 (en) |
EP (1) | EP1430357B1 (en) |
JP (1) | JP2005501295A (en) |
KR (1) | KR20040043096A (en) |
CN (1) | CN1473281A (en) |
CA (1) | CA2458635A1 (en) |
FR (1) | FR2829244B1 (en) |
TW (1) | TW574561B (en) |
WO (1) | WO2003019278A1 (en) |
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KR100882729B1 (en) | 2003-05-14 | 2009-02-06 | 엘지디스플레이 주식회사 | Liquid Crystal Display Device and the method of forming LCD |
FR2863061B1 (en) * | 2003-11-28 | 2006-02-24 | Nemoptic | WHITE OPTIMIZING NEMATIC SCREEN DISPLAY DEVICE AND METHOD OF DEFINING THE SAME |
FR2874446B1 (en) * | 2004-08-17 | 2007-01-12 | Nemoptic Sa | LIQUID CRYSTAL DISPLAY IMPROVES IN PARTICULAR BY REMOVING NEGATIVE EFFECTS ON EDGES OF ZONES ADDRESSED |
JP4675678B2 (en) * | 2005-05-27 | 2011-04-27 | シャープ株式会社 | Liquid crystal display element and manufacturing method thereof |
US8208080B2 (en) * | 2007-03-07 | 2012-06-26 | Chimei Innolux Corporation | Liquid crystal display |
EP2068195B1 (en) * | 2007-12-06 | 2010-04-14 | Nemoptic | Manufacturing method of a bistable liquid crystal display cell |
US9977909B1 (en) | 2015-01-13 | 2018-05-22 | State Farm Mutual Automobile Insurance Company | Selectively obscuring and/or revealing sensitive information in a display of a computing device |
US11500255B2 (en) | 2018-11-07 | 2022-11-15 | Alphamicron Incorporated | Variable transmission optical assembly having a pixelated switchable birefringent layer |
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US4239345A (en) * | 1979-04-16 | 1980-12-16 | Bell Telephone Laboratories, Incorporated | Bistable liquid crystal twist cell |
US5132816A (en) * | 1989-02-02 | 1992-07-21 | Sharp Kabushiki Kaisha | Ferroelectric liquid crystal device and method of manufacturing the same |
JPH055886A (en) * | 1991-06-27 | 1993-01-14 | Matsushita Electric Ind Co Ltd | Production of liquid crystal display element |
JPH063675A (en) * | 1992-06-24 | 1994-01-14 | Toshiba Corp | Liquid crystal display element and its manufacture |
JP3634390B2 (en) * | 1992-07-16 | 2005-03-30 | セイコーエプソン株式会社 | Liquid crystal electro-optic element |
GB9402492D0 (en) * | 1994-02-09 | 1994-03-30 | Secr Defence | Liquid crystal device alignment |
JPH07294933A (en) * | 1994-04-22 | 1995-11-10 | Seiko Epson Corp | Liquid crystal electro-optic element |
JPH08327969A (en) * | 1995-05-31 | 1996-12-13 | Sharp Corp | Liquid crystal display device |
FR2740894B1 (en) * | 1995-11-08 | 1998-01-23 | Centre Nat Rech Scient | IMPROVED DISPLAY DEVICE BASED ON LIQUID CRYSTALS AND WITH BISTABLE EFFECT |
JP3587426B2 (en) * | 1996-09-25 | 2004-11-10 | シャープ株式会社 | Liquid crystal display device and method of manufacturing the same |
JPH10333121A (en) * | 1997-06-03 | 1998-12-18 | Kyocera Corp | Liquid crystal display device |
JP3411199B2 (en) * | 1997-10-22 | 2003-05-26 | 株式会社アドバンスト・ディスプレイ | Liquid crystal cell manufacturing method |
JPH11174498A (en) * | 1997-12-08 | 1999-07-02 | Ricoh Co Ltd | Liquid crystal display device |
JPH11183879A (en) * | 1997-12-24 | 1999-07-09 | Kyocera Corp | Liquid crystal display device |
JPH11337946A (en) * | 1998-05-25 | 1999-12-10 | Kyocera Corp | Liquid crystal display device |
GB2350692A (en) * | 1999-05-15 | 2000-12-06 | Sharp Kk | Reflective liquid crystal device |
JP2000356791A (en) * | 1999-06-16 | 2000-12-26 | Ricoh Co Ltd | Liquid crystal display device |
FR2808891B1 (en) * | 2000-05-12 | 2003-07-25 | Nemoptic | BISTABLE REFLECTION DISPLAY DEVICE |
FR2808890B1 (en) * | 2000-05-12 | 2002-08-09 | Nemoptic | BISTABLE REFLECTION DISPLAY DEVICE WITH INVERSE CONTRAST |
-
2001
- 2001-08-29 FR FR0111227A patent/FR2829244B1/en not_active Expired - Fee Related
-
2002
- 2002-08-28 WO PCT/FR2002/002949 patent/WO2003019278A1/en active Application Filing
- 2002-08-28 TW TW091119601A patent/TW574561B/en not_active IP Right Cessation
- 2002-08-28 JP JP2003524083A patent/JP2005501295A/en active Pending
- 2002-08-28 CA CA002458635A patent/CA2458635A1/en not_active Abandoned
- 2002-08-28 EP EP02796319.8A patent/EP1430357B1/en not_active Expired - Lifetime
- 2002-08-28 CN CNA028027965A patent/CN1473281A/en active Pending
- 2002-08-28 US US10/488,223 patent/US7088413B2/en not_active Expired - Fee Related
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WO2003019278A1 (en) | 2003-03-06 |
JP2005501295A (en) | 2005-01-13 |
CN1473281A (en) | 2004-02-04 |
US20040201817A1 (en) | 2004-10-14 |
EP1430357A1 (en) | 2004-06-23 |
KR20040043096A (en) | 2004-05-22 |
US7088413B2 (en) | 2006-08-08 |
FR2829244A1 (en) | 2003-03-07 |
CA2458635A1 (en) | 2003-03-06 |
FR2829244B1 (en) | 2004-09-10 |
EP1430357B1 (en) | 2013-07-31 |
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